Please use this identifier to cite or link to this item:
http://hdl.handle.net/10397/5644
DC Field | Value | Language |
---|---|---|
dc.contributor | Department of Electrical Engineering | - |
dc.creator | Zhang, H | - |
dc.creator | Tang, DY | - |
dc.creator | Zhao, LM | - |
dc.creator | Tam, HY | - |
dc.date.accessioned | 2014-12-11T08:25:47Z | - |
dc.date.available | 2014-12-11T08:25:47Z | - |
dc.identifier.issn | 0146-9592 | - |
dc.identifier.uri | http://hdl.handle.net/10397/5644 | - |
dc.language.iso | en | en_US |
dc.publisher | Optical Society of America | en_US |
dc.rights | © 2008 Optical Society of America. This paper was published in Optics Letters and is made available as an electronic reprint with the permission of OSA. The paper can be found at the following URL on the OSA website: http://www.opticsinfobase.org/ol/abstract.cfm?uri=ol-33-20-2317. Systematic or multiple reproduction or distribution to multiple locations via electronic or other means is prohibited and is subject to penalties under law. | en_US |
dc.subject | Birefringence | en_US |
dc.subject | Fiber lasers | en_US |
dc.subject | Lasers | en_US |
dc.subject | Optical properties | en_US |
dc.subject | Polarization | en_US |
dc.subject | Ring lasers | en_US |
dc.title | Induced solitons formed by cross-polarization coupling in a birefringent cavity fiber laser | en_US |
dc.type | Journal/Magazine Article | en_US |
dc.description.otherinformation | Author name used in this publication: H. Y. Tam | en_US |
dc.identifier.spage | 2317 | - |
dc.identifier.epage | 2319 | - |
dc.identifier.volume | 33 | - |
dc.identifier.issue | 20 | - |
dc.identifier.doi | 10.1364/OL.33.002317 | - |
dcterms.abstract | We report on the experimental observation of induced solitons in a passively mode-locked fiber ring laser with a birefringence cavity. Owing to the cross coupling between the two orthogonal polarization components of the laser, it was found that if a soliton was formed along one cavity polarization axis, a weak soliton was also induced along the orthogonal polarization axis, and depending on the net cavity birefringence, the induced soliton could have either the same or different center wavelengths to that of the inducing soliton. Moreover, the induced soliton always had the same group velocity as that of the inducing soliton. They formed a vector soliton in the cavity. Numerical simulations confirmed the experimental observations. | - |
dcterms.accessRights | open access | en_US |
dcterms.bibliographicCitation | Optics letters, 15 Oct. 2008, v. 33, no. 20, p. 2317-2319 | - |
dcterms.isPartOf | Optics letters | - |
dcterms.issued | 2008-10-15 | - |
dc.identifier.isi | WOS:000260970800012 | - |
dc.identifier.scopus | 2-s2.0-55349090630 | - |
dc.identifier.eissn | 1539-4794 | - |
dc.description.oa | Version of Record | en_US |
dc.identifier.FolderNumber | OA_IR/PIRA | en_US |
dc.description.pubStatus | Published | en_US |
dc.description.oaCategory | VoR allowed | en_US |
Appears in Collections: | Journal/Magazine Article |
Files in This Item:
File | Description | Size | Format | |
---|---|---|---|---|
Zhang_Solitons_Birefringent_Cavity.pdf | 195.08 kB | Adobe PDF | View/Open |
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